Event generation with Sherpa 2.2
Sherpa is a general-purpose Monte Carlo event generator for the simulation of particle
collisions in high-energy collider experiments. We summarize essential features and …
collisions in high-energy collider experiments. We summarize essential features and …
[HTML][HTML] Luminosity determination in pp collisions at = 8 TeV using the ATLAS detector at the LHC
M Aaboud, G Aad, B Abbott, J Abdallah… - The European Physical …, 2016 - Springer
The luminosity determination for the ATLAS detector at the LHC during pp collisions at s= s=
8 TeV in 2012 is presented. The evaluation of the luminosity scale is performed using …
8 TeV in 2012 is presented. The evaluation of the luminosity scale is performed using …
[HTML][HTML] Fully differential NNLO computations with MATRIX
M Grazzini, S Kallweit, M Wiesemann - The European Physical Journal C, 2018 - Springer
We present the computational framework Matrix (http://matrix. hepforge. org/) which allows
us to evaluate fully differential cross sections for a wide class of processes at hadron …
us to evaluate fully differential cross sections for a wide class of processes at hadron …
Multiboson interactions at the LHC
DR Green, P Meade, MA Pleier - Reviews of Modern Physics, 2017 - APS
This review covers results on the production of all possible electroweak boson pairs and 2-to-
1 vector boson fusion at the CERN Large Hadron Collider (LHC) in proton-proton collisions …
1 vector boson fusion at the CERN Large Hadron Collider (LHC) in proton-proton collisions …
Rethinking jets with energy correlators: Tracks, resummation, and analytic continuation
We introduce an infinite set of jet substructure observables, derived as projections of N-point
energy correlators, that both are convenient for experimental studies and maintain …
energy correlators, that both are convenient for experimental studies and maintain …
[HTML][HTML] Consistency of the standard model effective field theory
We derive bounds on couplings in the standard model effective field theory (SMEFT) as a
consequence of causality and the analytic structure of scattering amplitudes. In the SMEFT …
consequence of causality and the analytic structure of scattering amplitudes. In the SMEFT …
Les Houches 2011: physics at TeV colliders new physics working group report
G Brooijmans, B Gripaios, F Moortgat… - arXiv preprint arXiv …, 2012 - arxiv.org
We present the activities of the" New Physics" working group for the" Physics at TeV
Colliders" workshop (Les Houches, France, 30 May-17 June, 2011). Our report includes new …
Colliders" workshop (Les Houches, France, 30 May-17 June, 2011). Our report includes new …
Future physics opportunities for high-density QCD at the LHC with heavy-ion and proton beams
Z Citron, A Dainese, JF Grosse-Oetringhaus… - arXiv preprint arXiv …, 2018 - arxiv.org
The future opportunities for high-density QCD studies with ion and proton beams at the LHC
are presented. Four major scientific goals are identified: the characterisation of the …
are presented. Four major scientific goals are identified: the characterisation of the …
Electroweak precision tests in high-energy diboson processes
R Franceschini, G Panico, A Pomarol, F Riva… - Journal of High Energy …, 2018 - Springer
A bstract A promising avenue to perform precision tests of the SM at the LHC is to measure
differential cross-sections at high invariant mass, exploiting in this way the growth with the …
differential cross-sections at high invariant mass, exploiting in this way the growth with the …
[HTML][HTML] Measurement of the inclusive and differential t $$\overline {t} $$ γ cross sections in the dilepton channel and effective field theory interpretation in proton …
A Tumasyan, W Adam, JW Andrejkovic… - Journal of High Energy …, 2022 - Springer
A bstract The production cross section of a top quark pair in association with a photon is
measured in proton-proton collisions in the decay channel with two oppositely charged …
measured in proton-proton collisions in the decay channel with two oppositely charged …